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Defense Intelligence Reference Document Inertial Electrostatic Confinement Fusion

Defense Intelligence Agency · 72 pages · text from the file's own layer

This Defense Intelligence Agency reference document, dated 10 March 2010, covers inertial electrostatic confinement (IEC) fusion. It was produced in FY 2009 under the DIA's Advanced Aerospace Weapon System Applications (AAWSA) program. The report focuses on work at the University of Illinois Urbana-Champaign and reviews IEC basics, experiments, theory and applications such as neutron sources, explosives detection and space propulsion. It concludes by proposing a breakeven experiment for p-11B fusion that uses a hydrogen plasma simulation.

  • p. 5 …Sketch of Two Opposite Limits of the Beam·Maxwellian Equilibrium .. 38 Figure 4.5. The Definition…
  • p. 6 …Comparison of Analytical and Numerical Estimates of Q-Values in a Beam-Dominated Solution -- for a…
  • p. 8 …shows the "Star Mode" discharge where ion beams are created that pass through the grid openings…
  • p. 9 …discussed later where the recirculating ions possess beam-like trajectories passing through the center of the…
  • p. 10 UNCLASSIFIED/ ;raA 8FFIIItliL ~81!! SHL'f beam-like ions. Since electron energy loss processes such as…
  • p. 11 …In addition, its beam-like reactions (highly non-Maxwellian) make the IEC very well suited for…
  • p. 13 …a beam created at the anode and accelerated by the applied cathode voltage; a low-energy…
  • p. 14 …Good convergence is required to achieve optimal beam-beam reactivity scaling for the application that require…
  • p. 15 …The observed loss of convergence with decreasing pressure and increasing current makes achieving significant beam-beam…
  • p. 16 …For a power reactor the objective is to obtain ion beam-beam collisions in this central…
  • p. 17 …the "conventional" beam-like one. A key issue for this concept is how much plasma compression…
  • p. 19 …The main beam observed is a direct path along the injector angle. Other faint light channels…
  • p. 21 …Note that six ion "guns" were used to create a low energy ion beam that entered…
  • p. 22 UNCLASSIFIED/;SflHl 8FFIIItliL ~81!! 8HL'I' was obtained from recirculation beam-beam reactions in a potential…
  • p. 23 …The key physics point is that the beam-beam fusion rate scales as the ion current…
  • p. 26 …Scoping calculations of beam-background fusion rates predict that a 3 He- 3 He reaction product…
  • p. 27 …of the ion density squared scaling for beam-beam reactions. REFERENCES 2.1 R. L. Hirsch…
  • p. 28 …As such, the beam convergence (compression) is limited to lower values, hence lower core densities (an…
  • p. 30 …by the intersection of the multiple ion beams, serves to deflect ions into the escaping jet…
  • p. 31 …The result is the formation of the intense space charge neutralized ion beam (or "plasma jet…
  • p. 32 …in the symmetric microchannels into a directed beam or jet. Comparison to a Conventional "Plasma" Thruster…
  • p. 33 …The ion beams finally exit through an opening in the ground sphere of the IEC device…
  • p. 35 …These devices operate with ~ 80- keV D-ion beams using the non-Maxwellian character of the…
  • p. 36 …Two ion sources inject 40-keV deuterium and helium-3 ion beams toward the center of…
  • p. 37 …Indeed in this case fusion is dominated by beam-beam (non- Maxwellian reactions). Also, the dipole…
  • p. 38 …the center potential and consequently allow incoming beam ions to penetrate into the core region. In…
  • p. 39 …Comparison of Analytical and Numerical Estimates of Q-values in a beam-Dominated Solution -- for a…
  • p. 40 …Hora, "Converging Beam Neutron Source for Driving a Sub-critical Fission Reactor", Proceedings, ICONE 8, CD…
  • p. 41 …Namely, the time scale for collisional degradation of the beam-like ion distribution function is crucial…
  • p. 42 …For example, a tightly focused monoenergetic ion beam is in fact a pessimistic scenario, because different…
  • p. 44 …Thus, weak sinks and strong sources will result in a large beam population, increasing the beam…
  • p. 45 …Sketch of Two Opposite Limits of the Beam-Maxwellian Equilibrium. The solid line corresponds to a…
  • p. 46 …injected beam current, average injection energy, energy spread associated with the velocity component in both parallel…
  • p. 47 …As stated in Section I, the current scaling for beam-beam reactions is strictly 12. However…
  • p. 48 …is very encouraging for formation of deep wells in IEC devices designed for reactors using beam…
  • p. 49 …To do this, it is assumed that the electrostatic confinement equilibrium ion beams are proportional to…
  • p. 50 …When an ion beam is hot, the waves excited by the instability are ion acoustic type…
  • p. 51 …Rider was particularly interested in the claim that due to its beam-like non- Maxwellian plasma…
  • p. 52 …Diagram Showing Equipotential Surfaces of the IEC Cathode Grid and Their Focusing Effect on a Beam…
  • p. 59 …of detectors, the detector configuration, the collimated beam size, the acquisition time, and other scan-related…
  • p. 63 …Alternately, for space propulsion, the proton beam, augmented by injection of heavy atoms to increase the…
  • p. 68 …Due to its inherent non-Maxwellian (beam-like) plasma, the IEC is especially well suited for…
  • p. 70 …This configuration is highly non-Maxwellian due to the beam dominated nature of the trapped ions…
UNCLASSIFIED/;Sf81il 8FFIIItliL ~81!! 8HLY
plasma. When an ion beam is hot, the waves excited by the instability are ion acoustic
type waves. Then one observes that a certain temperature ratio is required before the
wave will go unstable.
He also developed a two-dimensional perturbative (i5f) particle-in-cell algorithm to
simulate the electrostatic interaction of electrons and ions in spherical inertial
electrostatic confinement. i5f scheme is applied, because the noise level in i5f algorithm
is significantly reduced, compared with conventional particle-in-cell simulation. Since a
particle-in-cell simulation in two or three-dimensions is very computationally and
memory intensive, it is necessary to seek computational methods and options which
lead to solutions in a reasonable amount of time. A distributed computing approach is
implemented by using parallel libraries. Applying a uniform grid spacing in spherical
coordinates may lead to a stability problem due to singularity at the spherical center. In
order to avoid the singularity issue, a two-dimensional rectangular domain and an
immersed boundary method are applied so that a spherical domain inside the cathode
gird of spherical electrostatic confinement is simulated by r-z coordinates. It is evident
from the result that the growth rate of instability, a decreasing function of the
longitudinal energy spread of ion distribution function, becomes reduced because the
large energy spread induces strong Landau damping by parallel kinetic effects. Besides
the effects of longitudinal Landau damping by the barn ions, a more monoenergetic
beam is able to stabilize the instability because a growth rate of instability can be
reduced for a higher beam density when the beam speed is fixed and located on the left
hill in the diagram of growth rate versus beam speed. The growth rate does not change
dramatically as a mode of angular perturbation increases.
The results summarized in Figure 4.10 indicated that the two-stream instability is
stabilized if the angular momentum spread of the beam ions is small enough, due to
enhanced ion densification at the center of the device. This is very encouraging for
future IEC development. However, an experimental study should be performed to verify
this result.
RIDER - ENERGY BALANCE STUDY
Todd Rider in Reference 4. 7 reports a quite different type of energy balance analysis.
While the prior papers used various methods to concentrate on up-down scattering in
various potential well configurations, Rider considered a "block diagram" type energy
flow balance to determine the net gain from a power unit. In such an analysis the
reaction and scattering rates, plus the electron-ion equilibration rates, enter as ()
averaged over the distribution functions for ions and electrons. Thus, the distribution
functions were not calculated explicitly in Rider's analysis. In addition to the base
function, any spatial variations in the distribution, such as pointed out by Tzonev et al.,
must be envisioned via the assumed distribution function. In traditional magnetic
confinement analyses a Maxwellian distribution function has generally been assumed.
In prior Tokamak studies, this technique has been widely used with reasonable
accuracy since such systems are indeed near thermal equilibrium. In sharp contrast, as
stressed repeatedly here, the IEC is not.
This uncertainly in makes an analysis of the type attempted by Rider very
challenging, and leaves it open for possible criticism. In fact, it appears that Rider used
Maxwellian key averages and critics generally cite this as the cause for his pessimistic
43
UNCLASSIFIED/,'f81il 8ffll1Als WliEii &••blf

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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 72 pages are in the text index: search them above, or from the library's search.